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cond1.dvi
www.damtp.cam.ac.uk/user/na/people/Alexei/papers/cond1.pdf1 Sep 2011: More details on the problems relevant to k;p can befound in [1],[2],[5].Recall that Nj(t) := (tjk tj) [tj; tj1; : : :; tjk] ( t)k1+ ;so that suppNj = (tj; tjk); ... degree p such thatsuppMj;p = (tj; tjp1); Z tjp1tj Mj;p(x)dx = 1;and by! -
cond2.dvi
www.damtp.cam.ac.uk/user/na/people/Alexei/papers/cond2.pdf1 Sep 2011: 2. Condition number and related constantsLet fN̂jg be the B-spline basis of order k on a knot sequence t = (tj), tj < tjk,normalized with respect to the Lp-norm (1 ... p 1), i.e.,N̂j(x) = (k=(tjk tj))1=pNj(x);where fNjg is the B-spline basis which -
shadrin.dvi
www.damtp.cam.ac.uk/user/na/people/Alexei/papers/mon.pdf1 Sep 2011: x) : 1(yi1) = g(yi1); 01(yi1) = g0(yi1+);ki1(x) : ki1(yi) = g(yi); 0ki1(yi) = g0(yi);and for j such that Tj = Tj ,j(x) : 8><>: (r)j ... Hence 2 S(A0i;1); A0i 2 Xj: Tj=Tj 1:Since i(x) = maxf(x); p(x)g;we change into p at most once in each T j. -
spn0.dvi
www.damtp.cam.ac.uk/user/na/people/Alexei/papers/spn0.pdf1 Sep 2011: The subintervals of and their lengthes will be denoted by. Ij := (tj, tj1), |hj| := tj1 tj. ... Nj = 1, (1.1.1). Mj (x) =k. tjk tjNj(x),. tjk. tj. -
revision.dvi
www.damtp.cam.ac.uk/user/na/people/Alexei/papers/kmon.pdf1 Sep 2011: f (tj ) = g(tj ) on {a = t0 < t1 <. < tn < tn1 = b}. Then, there exists a spline z such that. ... be such thatg(tj ) = p(tj ) on {a = t0 < t1 <. < tn < tn1 = b}. Then, there exists a spline z such that. -
348_2007_387_43_5-web 737..753
www.damtp.cam.ac.uk/user/gold/pdfs/eif.pdf10 Apr 2011: R E S E A R C H A R T I C L E. Fluid dynamics of self-propelled microorganisms,from individuals to concentrated populations. Luis H. Cisneros Æ Ricardo Cortez ÆChristopher Dombrowski Æ Raymond E. Goldstein ÆJohn O. Kessler. Received: 13 February -
Phenomenological theory of multiply reentrant solubility Raymond E.…
www.damtp.cam.ac.uk/user/gold/pdfs/JChemPhys_83_1246.pdf10 Apr 2011: tJ.Se(T,Hcrit ) = Se(T,H--Hcrit ) - Se(T,H--Hcrit -). (17). where.tJ.Ms is the order parameter jump of the SM. ... tJ.Me(T ,Hcrit) = Me(T ,H--Hcrit ) - Me(T ,H--Hcrit -). (18). -
201019079 10940..10945
www.damtp.cam.ac.uk/user/gold/pdfs/noise.pdf6 Jul 2011: Phys Rev E Stat Nonlin Soft Matter Phys 80:041922.22. Ishikawa T, Locsei JT, Pedley TJ (2008) Development of coherent structures in concen-. ... Science 325:487–490. 43. Pedley TJ, Kessler JO (1992) Hydrodynamic phenomena in suspensions of -
Microfluidics of cytoplasmic streaming and itsimplications for…
www.damtp.cam.ac.uk/user/gold/pdfs/streaming_pnas.pdf10 Apr 2011: Magar V, Goto T, Pedley TJ (2003) Q J Mech Appl Math 56:65–91.35. -
201019079 7..12
www.damtp.cam.ac.uk/user/gold/pdfs/noise_SI.pdf6 Jul 2011: 1. Pedley TJ, Kessler JO (1992) Hydrodynamic phenomena in suspensions of swimmingmicroorganisms. -
MMB160.indd
www.damtp.cam.ac.uk/user/gold/pdfs/spirochete_review.pdf10 Apr 2011: Nature 2001; 413: 39–44. Wilson DR, Beveridge TJ: Bacterial f lagellar fila-ments and their component f lagellins. -
201019079 1..6
www.damtp.cam.ac.uk/user/gold/pdfs/PNAS-2011-Drescher-1019079108.pdf20 Jun 2011: Phys Rev E Stat Nonlin Soft Matter Phys 80:041922.22. Ishikawa T, Locsei JT, Pedley TJ (2008) Development of coherent structures in concen-. ... Science 325:487–490. 43. Pedley TJ, Kessler JO (1992) Hydrodynamic phenomena in suspensions of -
msr124 2921..2933
www.damtp.cam.ac.uk/user/gold/pdfs/b12.pdf27 Sep 2011: Insights into the Evolution of Vitamin B12 Auxotrophy fromSequenced Algal Genomes. Katherine E. Helliwell,1 Glen L. Wheeler,2,3 Kyriacos C. Leptos,4 Raymond E. Goldstein,4 andAlison G. Smith,1. 1Department of Plant Sciences, University of Cambridge, -
Generalized sampling and the stable and accuratereconstruction of…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2011_12.pdf22 Nov 2011: Tj(x) = cos(j arccos x), j = 0, 1, 2,. ,. and c0 = 1π , cj =. 2π , j 6= 1. ... Given that the polynomials Tj are orthogonal with respect to the weight. -
J. Phys. II France 6 (1996) 767-796 MAY 1996, ...
www.damtp.cam.ac.uk/user/gold/pdfs/gnps.pdf10 Apr 2011: J. Phys. II France 6 (1996) 767-796 MAY 1996, PAGE 767. Front Propagation in the Pearling Instability of Tubular Vesicles. Raymond E. Goldstein (), Philip Nelson (), Thomas Powers (>)and Udo Seifert (). () Joseph Henry Laboratory of Physics, -
PART I: Symmetries and particles. NOTES BY PROF. HUGH ...
www.damtp.cam.ac.uk/user/examples/3P2Lb.pdf10 Oct 2011: PART I: Symmetries and particles. NOTES BY PROF. HUGH OSBORN. Books. Books developing group theory by physicists from the perspective of particle physics are. H. F. Jones, Groups, Representations and Physics, 2nd ed., IOP Publishing (1998).A fairly -
DAMTP 2010/NA04 Beyond symmetric Broyden for updating quadratic…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2010_04.pdf13 Apr 2011: F(x) = 12xT{ n. j=1 100(j1)/(n1) vj v. Tj. }x, xRn. -
Continuum theory of critical phenomena in polymer solutions:…
www.damtp.cam.ac.uk/user/gold/pdfs/JChemPhys_90_7448.pdf10 Apr 2011: Continuum theory of critical phenomena in polymer solutions: Formalism and mean field approximation. Raymond E. Goldstein Laboratory of Atomic and Solid State Physics and Materials Science Center, Clark Hall, Cornell University, Ithaca, New York -
Physics of chemoreception
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/bergpurcell.pdf6 Oct 2011: 52 predicts for a single receptor if IJ = TJ(1 - p). -
g.dvi
www.damtp.cam.ac.uk/user/na/people/Alexei/papers/markov.pdf1 Sep 2011: APPROXIMATION THEORY:A volume dedicated to Borislav Bojanov(D. K. Dimitrov, G. Nikolov, and R. Uluchev, Eds.)additional information (to be provided by the publisher). Twelve Proofs of the Markov Inequality. Aleksei Shadrin. This is the story of the
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